1.

The solution of the partial differential equation \(\frac{{\partial u}}{{\partial t}} = \alpha \frac{{{\partial ^2}u}}{{\partial {x^2}}}\) is of the form

A. \(C\cos \left( {kt} \right){C_1}{e^{\left( {\sqrt {\frac{k}{\alpha }} } \right)x}} + {C_2}{e^{ - \left( {\sqrt {\frac{k}{\alpha }} } \right)x}}\)
B. \(C{e^{kt}}[{C_1}{e^{\left( {\sqrt {\frac{k}{\alpha }} } \right)x}} + {C_2}{e^{ - \left( {\sqrt {\frac{k}{\alpha }} } \right)x}}]\)
C. \(C{e^{kt}}{C_1}\cos \left( {\sqrt {\frac{k}{\alpha }} } \right)x + {C_2}\sin \left( { - \sqrt {\frac{k}{\alpha }} } \right)x\)
D. \(C\sin \left( {kt} \right){C_1}\cos \left( {\sqrt {\frac{k}{\alpha }} } \right)x + {C_2}\sin \left( { - \sqrt {\frac{k}{\alpha }} } \right)x\)
Answer» C. \(C{e^{kt}}{C_1}\cos \left( {\sqrt {\frac{k}{\alpha }} } \right)x + {C_2}\sin \left( { - \sqrt {\frac{k}{\alpha }} } \right)x\)


Discussion

No Comment Found